/*===================================================================*/ /* NRDF D0152 Data No.3 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,3; D#=D152; TITLE=/(P,D) REACTIONS AT 52 MEV.I.58NI(P,D)57NI (EXPERIMENTAL)/; PURPOSE=/TO TEST THE VALIDITY OF CURRENT REACTION THEORIES,(P,D)ANGULAR DISTRIBUTION HAVE BEEN TAKEN AT THE INCIDENT ENERGY OF 52MEV, THE HIGHEST ENERGY SO FAR STUDIED,OVER A WIDE RANGE OF ANGLES AND IN SMALL STEPS'D'/; ATH=(H.OHNUMA'C',T.SUEHIRO'A,C',M.SEKIGUCHI'C',S.YAMADA'B,C'); INST-ATH=(2JPNINS'C'); /* 'A' PRESENT ADRESS:TOHOKU INSTITUTE OF TECHNOLOGY */ /* 'B' PRESENT ADRESS: TOKYO INSTITUTE OF TECHNOLOGY */ REF=JPJ; VLP=36(1974)1236; RCTS=(58NI(P,D)57NI); /* 'D'THE 58NI(P,D)REACTION,WHICH WE BELIEVE REQUIRE ANALYSIS FROM VARIOUS ASPECTS. BRIET DESCRIPTION OF ANALYSIS AND SPECTIOSCOPIC INFORMATION OBTAINED ARE ALSO GIVEN. DETAILS OF THE ANALYSIS WE HAVE DONE SO FAR WILL BE GIVEN IN A SUBSEQUENT PAPER: H.OHNUMA ET AL., J .PHYS.SOC.JAPAN 36(1974)1245 */ /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,3; RCT=58NI(P,D)57NI; CHM=ELM; THK-TGT=2.7MG/CM**2; BAC=SELF; ACC=(SYNCYC); INST-ACC=2JPNINS; INC-ENGY-RANGE=(51.93MEV); DET-PARTCL=(D); DET-SYS=(D); DET-SYS=(MAG+PROP-CNTR); ERS-DET=70KEV; ANL=(OPT-MODEL,DWBA); PHQ=(ANGL-DSTRN); /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,3; INC-ENGY=51.93MEV; THTC=5.8[110.3DEG; EXC-ENGY=0.76MEV; J-PI=5/2-; TRANSF-L=[3; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (MB/SR) (MB/SR) 6.0 1.06 0.02 8.0 1.00 0.02 10.6 0.92 0.02 13.1 0.90 0.03 15.7 0.79 0.02 18.3 0.66 0.02 20.8 0.49 0.01 23.4 0.36 0.01 26.0 0.26 0.01 28.5 0.21 0.01 31.1 0.21 0.01 33.7 0.21 0.01 36.2 0.195 0.006 38.8 0.143 0.005 41.3 0.116 0.004 43.9 0.088 0.004 46.4 0.079 0.003 49.0 0.089 0.004 51.5 0.090 0.004 54.1 0.097 0.004 56.6 0.086 0.003 59.1 0.075 0.003 61.7 0.055 0.003 64.2 0.044 0.003 66.7 0.034 0.002 69.3 0.034 0.002 71.8 0.030 0.002 74.3 0.028 0.002 76.8 0.024 0.002 79.4 0.025 0.002 81.9 0.023 0.002 86.9 0.015 0.0015 91.9 0.012 0.0013 96.9 0.0082 0.0012 101.9 0.0066 0.0010 106.8 0.0042 0.0008 111.8 0.0035 0.0008 \END; /*===================================================================*/ |